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[PDF] Top 20 Lat. Am. j. solids struct. vol.11 número13

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Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... of Solids and Structures 11 (2014) 2308-2332 Experimental investigation on propagation of incident irregular waves over a submerged bar is car- ried out by Beji and Battjes (1993) and its numerical ... See full document

25

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... Latin American Journal of Solids and Structures 11 (2014) 2408-2425 SAW devices and more recently nondestructive evaluation. The study of surface wave propagation is of much practical importance in various ... See full document

18

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... Latin American Journal of Solids and Structures 11 (2014) 2333-2350 Again, firstly the results for a balanced shaft are plotted in Figure 10. Here, the percentage of opening has been plotted versus angle of ... See full document

18

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... Comparison of peak central point displacements of the sandwich foam panels with 50, 100, and 150 mm thick foam core with different relative densities show that the panels with foam rela[r] ... See full document

19

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... The propagation characteristic of shear wave based on dispersion relation derived in equation (27) is investigated by numerically analysis carried out in this section for two different [r] ... See full document

14

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... of Solids and Structures 11 (2014) 2460-2482 Gold Nano-Beams based nano-carriers have great potential in biomedical fields, such as biologi- cal monitoring, imaging, thermotherapy and multifunctional ... See full document

23

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... of Solids and Structures 11 (2014) 2444-2459 where Ψ is the free energy density, ε is the strain tensor, σ is the stress tensor and C is the elastic ... See full document

16

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... g = nm , respectively. It is understood that for all gaps above 15 nm there are three fixed points before pull-in voltage. One of them is under the substrate which is physically impossible, but other two points are above ... See full document

18

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... of Solids and Structures 11 (2014) 2379-2407 Thickness of the composite panels is one of the most efficient parameters in noise transfer; therefore according to Figure 13, the influence of this parameter on ... See full document

29

Lat. Am. j. solids struct.  vol.11 número13

Lat. Am. j. solids struct. vol.11 número13

... of Solids and Structures 11 (2014) 2351-2378 value of non-dimensional length scale parameter shifts the postbuckling curves to the left-hand side, resulting in lower critical applied loads and higher ... See full document

28

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... Latin American Journal of Solids and Structures 11 (2014) 2537-2554 As mentioned in Subsection 3.1, the choice of number of Trefftz functions, m , which may affect the accuracy and convergence of the ... See full document

18

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... In the third simulation, the autonomous vehicle and the obstacle are both moving on a circular road of 500 meter radius. The forward velocities are similar to those of the first simulation. The differ- ence between the ... See full document

18

Lat. Am. j. solids struct.  vol.13 número13

Lat. Am. j. solids struct. vol.13 número13

... In the present context, we do not intend to characterize all possible vibrational modes of the nonlinear bubble oscillatory motion, as done in previous works (Malvar, 2014). Our goal is[r] ... See full document

26

Lat. Am. j. solids struct.  vol.13 número13

Lat. Am. j. solids struct. vol.13 número13

... Solution abstract class starts the solution process and has the necessary resources for solving the matrix system. GFEM gl process is implemented by GlobalLocal class, as shown in Fig. 4. Since GFEM gl is composed by ... See full document

23

Lat. Am. j. solids struct.  vol.13 número13

Lat. Am. j. solids struct. vol.13 número13

... (3) There are differences in the dynamic responses based on the single-layer and double-layer track models, and the differences in both the maximum lateral and vertical dynamic response[r] ... See full document

39

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... Latin American Journal of Solids and Structures 11 (2014) 2573-2588 one at the midpoint of each segment, and vibrations were excited by giving it manual impulse force. Impulse force in different ... See full document

16

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... Latin American Journal of Solids and Structures 11 (2014) 2607-2623 The history of the contact force between the ball and the plate is shown in Figure 8(a). It can be seen that after they contact each ... See full document

17

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... In this study, two types of mesh will be used, as they are shown in Figs. (14-2) and (14-3). The quadrilaterals are generally divided into two triangles in the shortest-diagonal-cut of the Mesh A. To check the ... See full document

24

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... of Solids and Structures 11 (2014) 2624-2647 Further, the effect of the wear depth on the journal surface is illustrated in Figure 15, where the initial and final geometric configurations are presented and ... See full document

24

Lat. Am. j. solids struct.  vol.11 número14

Lat. Am. j. solids struct. vol.11 número14

... Figures 10 and 11 reveals that the variation of quality factor with the dimensionless frequency for the flexural symmetric modes with and without thermal signal. The quality factor is quite high at lower range of ... See full document

18

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